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Embedded-Atom Potentials

An extended discussion on embedded-atom potentials necessary for MD calculations can also be found (49). [Pg.397]

Dislocation core structures of (100), (110) and (111) dislocations in NiAl have been studied by molecular statics calculations using a new many-body embedded atom potential. They... [Pg.353]

This concept of metallic cohesion as arising from embedding ions in a gas of free electrons suggests that the binding energy of a collection of atoms with position vectors Rf may be approximated in the form of an embedded atom potential, namely... [Pg.131]

Embedded atom potentials have been extensively used for performing atomistic simulations of point, line and planar defects in metals and alloys (e.g. Vitek and Srolovitz 1989). The pair potential ( ), atomic charge density pBtom(r), and embedding function F(p) are usually fitted to reproduce the known equilibrium atomic volume, elastic moduli, and ground state structure of the perfect defect-free lattice. However, the prediction of ground state structure, especially the competition between the common metallic structure types fee, bcc, and hep, requires a more careful treatment of the pair potential contribution ( ) than that provided by the semiempirical embedded atom potential. This is considered in the next chapter. [Pg.134]

Thus, the total binding energy per atom of a NFE metal can be expressed in a physically transparent form, as the sum of a volume-dependent contribution and a pair-potential contribution in a manner that is reminiscent of the semi-empirical embedded atom potential of eqn (5.68). It follows from eqs (6.59M6.72) that... [Pg.151]

M.I. Baskes et al Semiempirical modified embedded-atom potentials for silicon and germanium. Physl. Rev. B 40, 6085-6100 (1989)... [Pg.130]

In our own work,33 that we here shall discuss briefly, we used the embedded-atom potential together with the Aufbau/Abbau method of Section 2.8 in optimizing the structure. The stability function, A2E(N), Eq. (50), is shown in Figure 18. It shows a set of peaks that correspond to particularly stable clusters. It is interesting to notice that if one instead studies the total-energy difference... [Pg.290]

Baskes. M. I.. Modified embedded-atom potentials for cubic materials and impurities. Phys. Rev. B 46, 2727-2742 (1992). [Pg.292]

This so-called embedded atom potential consists of two terms. The first term is a two-body potential that represents the repulsion between the ion and the rest of the ions in the system. The second term is a many-body function that represents the energy to embed an atom in the position i, where there is an electron density p that comes from the linear superposition of spherically averaged atomic electron densities. [Pg.82]

Fig. 1.9. Dislocation core in A1 as seen experimentally using high-resolution transmission electron microscopy (a) and image simulation of results of atomistic simulation using embedded-atom potentials (b) (adapted from Mills et al. (1994)). Fig. 1.9. Dislocation core in A1 as seen experimentally using high-resolution transmission electron microscopy (a) and image simulation of results of atomistic simulation using embedded-atom potentials (b) (adapted from Mills et al. (1994)).
Fig. 5.14. Energy as a function of volumetric strain as computed using atomic-scale analysis in terms of embedded-atom potentials (courtesy of D. Pawaskar). The atomistic result is compared with the quadratic fit like that suggested in eqn (5.93). Fig. 5.14. Energy as a function of volumetric strain as computed using atomic-scale analysis in terms of embedded-atom potentials (courtesy of D. Pawaskar). The atomistic result is compared with the quadratic fit like that suggested in eqn (5.93).
Using the Cauchy-Born rule in conjunction with the Johnson embedded-atom potential, compute the energy of a shearing deformation on (111) planes in the [110] direction. Show that the energy has the form given in fig. 2.14. [Pg.252]

Schwoebel Barrier on fee (111) Surfaces Using the Johnson embedded atom potential introduced in chap. 4, compute the energetics of an adatom in the vicinity of a step and derive results analogous to those given in fig. 11.2. [Pg.647]

Both the Finnis-Sinclair and the embedded-atom potentials (together with others that we have not considered here) can be represented using a very similar functional form. However, it is important to realise that they differ in the way that they connect to the first-principles, quantum mechanical model of bonding. They also differ in the procedures used to parametrise the models, so that different parametrisations may be reported for the same material. [Pg.244]

Embedded Atom potentials [95]. These are designed for simulations of metals and incorporate a simplified approximation of the local electron cloud density due to the presence of neighboring atoms. [Pg.15]

The Tight-Binding Model and Embedded-Atom Potentials... [Pg.157]

An elemental metal is described by three functions 0(R),p R) and F(p), while a binary system A-B requires seven functions 0aa, ab. bb. Pa[R), Pb(R), Fa(p), Fb(p). Over the past two decades the embedded-atom potentials have been constructed for many metals and a number of binary systems. EAM functions are usually defined by analytical expressions. The pair-interaction and electron-density functions are normally forced to vanish together with several higher derivatives at a cutoff radius R. Typically, Rc covers 3-5 coordination shells. [Pg.168]


See other pages where Embedded-Atom Potentials is mentioned: [Pg.262]    [Pg.341]    [Pg.142]    [Pg.131]    [Pg.131]    [Pg.133]    [Pg.134]    [Pg.134]    [Pg.529]    [Pg.413]    [Pg.505]    [Pg.328]    [Pg.341]    [Pg.358]    [Pg.341]    [Pg.239]    [Pg.900]    [Pg.166]    [Pg.167]   
See also in sourсe #XX -- [ Pg.4 , Pg.131 ]

See also in sourсe #XX -- [ Pg.358 ]

See also in sourсe #XX -- [ Pg.14 ]




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